Device and method for testing impedance characteristic and expansion performance of sound absorption material

ABSTRACT

Disclosed are a device and a method for testing impedance characteristic and expansion performance of a sound absorption material. The device includes a first cavity and a second cavity which are both sealed. The first cavity is communicated with the second cavity through a slit channel. The second cavity is used for placing a sound absorption material therein. The device further includes a sound excitation source whose sounding face is located in the first cavity and used to provide a testing sound pressure. The device further includes two sound pickup sensors whose sound pickup surfaces are respectively arranged in the first cavity and the second cavity and respectively used to detect sound pressure in the first cavity and the second cavity. The device further includes a material for enclosing the first cavity and the second cavity is a hard sound insulation material.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a U.S. National-Stage entry under 35 U.S.C. §371 based on International Application No. PCT/CN2015/081440 filed Jun. 15, 2015, and which claims priority to Chinese Application No. 201410713191.6, filed Nov. 28, 2014, which are all incorporated herein in their entirety by reference.

TECHNICAL FIELD

This application pertains to the technical field of material performance detection, and particularly to a device and a method for testing impedance characteristic and expansion performance of a sound absorption material.

BACKGROUND

A sound absorption material is a material having a strong performance of absorbing acoustic energy and reducing noise. When the sound absorption material is placed in a cavity, and a cavity is filled with sound pressure, the sound absorption material placed in the cavity absorbs partial acoustic energy, and this is equivalent to expanding a capacity of the cavity. Since the sound absorption material has such expansion characteristic, technician in the acoustic field place the sound absorption material in the cavities of some acoustic products to expand the capacity of the cavities of products without increasing external volume of the products, to improve the performance of acoustic products.

There are many kinds of materials capable of absorbing sound, but not every kind of sound absorption material has a very good expansion performance. To this end, technicians selects and uses a sound absorption material adapted for technical requirements of acoustic products from diverse sound absorption materials. However, currently there is not a device and a method for testing impedance characteristic and expansion performance of a sound absorption material. Technicians can only install each kind of sound absorption material into the acoustic product, then test to see whether the performance of the acoustic product changes or not, and thereby judge which sound absorption material is most adapted for the acoustic product. Such method of testing the sound absorption material is rather backward, causes large waste of manpower and material resources to enterprises, prolongs a development cycle of products, and thereby increases production costs of products.

In addition, other objects, desirable features and characteristics will become apparent from the subsequent summary and detailed description, and the appended claims, taken in conjunction with the accompanying drawings and this background.

SUMMARY

In view of the above drawbacks, the first technical problem to be solved by the present application is to provide a device for testing impedance characteristic and expansion performance of a sound absorption material. The device can test the impedance characteristic and expansion performance of the sound absorption material before it is installed in the acoustic product, thereby providing accurate technical indices for selection of the sound absorption material, eliminating waste of manpower and material resources, shortening the development cycle of acoustic products, and reducing the production costs of the product.

Based on a single general inventive concept, the second technical problem to be solved by the present application is to provide a method for testing impedance characteristic and expansion performance of a sound absorption material. By the method, the impedance characteristic and expansion performance of the sound absorption material can be accurately tested.

To solve the above first technical problem, the present application employs the following technical solutions:

A device for testing impedance characteristic and expansion performance of a sound absorption material comprises: a first cavity and a second cavity which are both sealed, the first cavity being communicated with the second cavity through a slit channel, wherein the second cavity is used for placing a sound absorption material therein; a sound excitation source whose sounding face is located in the first cavity and used to provide a testing sound pressure; two sound pickup sensors whose sound pickup surfaces are respectively arranged in the first cavity and the second cavity and which are respectively used to detect sound pressure in the first cavity and the second cavity; and a material for enclosing the first cavity and the second cavity is a hard sound insulation material.

Preferably, the first cavity and the second cavity each are a cavity with a regular shape.

Preferably, the sounding face of the sound excitation source flushes with a surface of an inner wall of the first cavity.

Preferably, the sound excitation source is a speaker.

Preferably, the sound pickup sensor is a microphone.

Preferably, the sound isolation material is one of metal, bakelite and acrylic.

To solve the above second technical problem, the present application employs the following technical solutions:

A method for testing impedance characteristic and expansion performance of a sound absorption material comprises the following steps:

S1: adjusting a voltage of the sound excitation source to enable the sound pressure in the second cavity to satisfy a sound pressure level needed by the test;

S2: Measuring a sound pressure P_(11(ω)) in the first cavity via the first sound pickup sensor, and measuring a sound pressure P_(21(ω)) in the second cavity via the second sound pickup sensor; solving an equivalent acoustic capacitance C_(a2) and an acoustic impedance Z_(a2(ω)) of the second cavity according to formula

${C_{a\; 2} = {{\frac{V_{2}}{\rho \; C_{0}^{2}}\mspace{14mu} {and}\mspace{14mu} Z_{a\; 2{(\omega)}}} = \frac{1}{\omega \; C_{a\; 2}}}},$

wherein V₂ is a volume of the second cavity, ρ is air density, C₀ is a sound speed, and ω is an angular speed;

S3: obtaining formula

$Z_{{ref}{(\omega)}} = \frac{P_{11{(\omega)}} - P_{21{(\omega)}}}{P_{21{(\omega)}} \times \omega \; C_{a\; 2}}$

according to an acoustic circuit that is equivalent to the device when the sound absorption material is not placed in the device, and putting the equivalent acoustic capacitance C_(a2) solved from step S2 into the formula to solve the acoustic impedance Z_(ref(ω)) of the slit channel;

S4: placing the sound absorption material to be tested in the second cavity, measuring a sound pressure P 12(ω) in the first cavity via the first sound pickup sensor, measuring a sound pressure P_(22(ω)) in the second cavity via the second sound pickup sensor, obtaining formula

$Z_{L{(\omega)}} = \frac{P_{22{(\omega)}}}{\frac{P_{12{(\omega)}} - P_{22{(\omega)}}}{Z_{{ref}{(\omega)}}}}$

according to the acoustic circuit that is equivalent to the device after the sound absorption material is placed in the device, putting the acoustic impedance Z_(ref(ω)) of the slit channel solved in step S3 into the formula to solve a uniform acoustic impedance Z_(L (ω)) after the sound absorption material is placed in the second cavity;

S5: obtaining formula

$Z_{L{(\omega)}} = \frac{\frac{1}{\omega \; C_{a\; 2}} \times \frac{1}{\omega \; C_{dut}}}{\frac{1}{\omega \; C_{a\; 2}} + \frac{1}{\omega \; C_{dut}}}$

according to the acoustic circuit that is equivalent to the device after the sound absorption material is placed in the device, and solving an equivalent acoustic capacitance C_(dut) of the sound absorption material; solving a capacity expansion amount V_(dut) of the sound absorption material according to the formula V_(dut)=ρC₀ ² C_(dut) , and thereby judging the impedance characteristic and expansion performance of the sound absorption material.

Wherein, a sound pressure level needed by the test in step S1 is a sound pressure level of an actual working environment of the sound absorption material.

The present application achieves the following advantageous effects after employing the above technical solutions:

In the present application, the device for testing impedance characteristic and expansion performance of the sound absorption material device comprises: a first cavity and a second cavity which are both sealed, the first cavity being communicated with the second cavity through a slit channel; a sound excitation source whose sounding face is located in the first cavity; two sound pickup sensors respectively used to detect sound pressure in the first cavity and the second cavity; and a material for enclosing the first cavity and the second cavity is a sound insulation material. When the performance of the sound absorption material is tested, the sound pressure in the first cavity and second cavity and the impedance of the slit channel are detected first, then the sound absorption material to be tested is placed in the second cavity, then the sound pressure in the first cavity and second cavity at this time is detected, then the equivalent acoustic capacitance and capacity expansion amount of the sound absorption material are solved from a formula which is obtained from an acoustic circuit equivalently worked out by the device at this time. Whether the sound absorption material satisfies technical requirements of the acoustic product may be judged according to the obtained equivalent acoustic capacitance and capacity expansion amount of the sound absorption material. Hence, the sound absorption material adapted for the acoustic product may be selected in a way that the sound absorption material needn't be installed in the acoustic product. This eliminates waste of manpower and material resources caused by test of sound absorption material for each acoustic product, substantially shortens the time for selecting the sound absorption material, thereby shortening a development cycle of a new product, reducing production costs of products and bringing about larger economic benefits to enterprises.

To conclude, the device and method for testing impedance characteristic and expansion performance of a sound absorption material according to the present application solve the technical problem in the prior art about difficulty in selecting the sound absorption material. The device and method for testing impedance characteristic and expansion performance of the sound absorption material according to the present application implement performance test of the sound absorption material, provide technical indices for selection of the sound absorption material, reduce the production costs of the acoustic product, and bring about larger economic benefits to the enterprises.

The above depictions are only generalization of technical solutions of the present application, which may be implemented according to content of the description to make technical means of the present application clearer. Specific embodiments of the present application are presented below to make the above and other objects, features and advantages of the present application more apparent.

BRIEF DESCRIPTION OF THE DRAWINGS

The present invention will hereinafter be described in conjunction with the following drawing figures, wherein like numerals denote like elements, and:

FIG. 1 is a structural schematic view of a device for testing impedance characteristic and expansion performance of a sound absorption material according to the present application;

FIG. 2 is an equivalent acoustic circuit diagram when the sound absorption material is not placed in the device for testing impedance characteristic and expansion performance of the sound absorption material according to the present application;

FIG. 3 is an equivalent acoustic circuit diagram after the sound absorption material is placed in the device for testing impedance characteristic and expansion performance of the sound absorption material according to the present application;

In the figures, the reference number 10 denotes first cavity, 20 denotes second cavity, 30 denotes slit channel, 40 denotes sound absorption material, 50 denotes sound excitation source, 60 denotes first sound pickup sensor, 62 denotes second sound pickup sensor, P₁₁, P₂₁ denote sound pressure of the first cavity, P₁₂, P₂₂ denote sound pressure of the second cavity, M_(a) denotes sound quality of the slit channel, R_(a) denotes acoustic impedance of the slit channel, C_(al) denotes equivalent acoustic capacitance of the first cavity, C_(a2) denotes equivalent acoustic capacitance of the second cavity, C_(dut) denotes equivalent acoustic capacitance of the sound absorption material.

DETAILED DESCRIPTION

The following detailed description is merely exemplary in nature and is not intended to limit the invention or the application and uses of the invention. Furthermore, there is no intention to be bound by any theory presented in the preceding background of the invention or the following detailed description.

The present application will be further illustrated with reference to figures and embodiments.

As shown in FIG. 1, a device for testing impedance characteristic and expansion performance of a sound absorption material comprises: a first cavity 10 and a second cavity 20 which are both sealed, wherein the first cavity 10 is communicated with the second cavity 20 through a slit channel 30. The device further comprises a sound excitation source 50 whose sounding face is located in the first cavity 10, and a first sound pickup sensor 60 whose sound pickup surface is located in the first cavity 10 and a second sound pickup sensor 62 whose sound pickup surface is located in the second cavity 20.

As shown in FIG. 1, both the first cavity 10 and second cavity 20 are a cavity of a regular shape such as cube, cuboid, cylinder or the like. Panel materials enclosing the first cavity 10 and second cavity 20 all are hard sound-isolating materials with strong reflectivity, for example, metallic, bakelite or acrylic plates with a thickness of over 2mm.

As shown in FIG. 1, in the present embodiment a speaker is selected as the sound excitation source 50 to provide sound pressure upon testing the sound absorption performance. A sounding face of the sound excitation source 50 flushes with the surface of the inner wall of the first cavity so that the sound pressure at all positions in the cavity is in equilibrium.

As shown in FIG. 1, in the present embodiment two high-sound pressure microphones are selected as the first sound pickup sensor 60 and the second sound pickup sensor 62 which are respectively used to detect the sound pressure in the first cavity 10 and the second cavity 20.

As jointly shown in FIG. 1 and FIG. 2, FIG. 2 is an equivalent acoustic circuit diagram when the sound absorption material is not placed in the device. The acoustic impedance

$Z_{a\; 2{(\omega)}} = \frac{1}{\omega \; C_{a\; 2}}$

of the second cavity 20 is solved from a capacitive reactance formula

${X_{C} = \frac{1}{\omega \; C}},$

Wherein, w is an angular speed,

C_(a) is an equivalent acoustic capacitance of the second cavity 20.

The acoustic impedance Z_(ref(ω)) of the slit channel 30 may be solved from FIG. 2,

$\begin{matrix} \begin{matrix} {Z_{{ref}{(\omega)}} = {{\omega \; M_{a}} + R_{a}}} \\ {= \frac{P_{11} - P_{21}}{\frac{P_{21}}{Z_{a\; 2}}}} \\ {= {\frac{P_{11} - P_{21}}{P_{21} \times \omega \; C_{a\; 2}}.}} \end{matrix} & {{formula}\mspace{14mu} (1)} \end{matrix}$

As jointly shown in FIG. 1 and FIG. 3, when the performance of the sound absorption material is tested, the sound absorption material 40 is placed in the second cavity 20, whereupon the acoustic circuit that is equivalent to the device after the sound absorption material is placed in the device is as shown in FIG. 3. A uniform acoustic impedance Z_(L(ω)) after the sound absorption material 40 is placed in the second cavity 20 may be solved according to the acoustic circuit diagram,

The acoustic impedance of the sound absorption material 40 is

$\begin{matrix} {{Z_{dut} = \frac{1}{\omega \; C_{dut}}},\begin{matrix} {Z_{L{(\omega)}} = \frac{Z_{a\; 2} \times Z_{dut}}{Z_{a\; 2} + Z_{dut}}} \\ {= \frac{\frac{1}{\omega \; C_{a\; 2}} \times \frac{1}{\omega \; C_{dut}}}{\frac{1}{\omega \; C_{a\; 2}} + \frac{1}{\omega \; C_{dut}}}} \end{matrix}} & {{formula}\mspace{14mu} (2)} \\ {{Z_{L{(\omega)}} = \frac{P_{22{(\omega)}}}{\frac{P_{12{(\omega)}} - P_{22{(\omega)}}}{Z_{{ref}{(\omega)}}}}},} & {{formula}\mspace{14mu} (3)} \end{matrix}$

As shown in FIG. 1, FIG. 2 and FIG. 3, the method of using the above testing device to test impedance characteristic and expansion performance of a sound absorption material comprises the following steps:

S1: calibrating the sound pressure in the second cavity 20, namely, detecting the sound pressure in the second cavity 20 via the second sound pickup sensor 62 by adjusting a voltage of the sound excitation source 50, so that the sound pressure in the second cavity 20 reaches a sound pressure level needed by the test. The sound pressure level needed by the test is consistent with the sound pressure level in the cavity of the acoustic product in which the sound absorption material is to be installed, namely, a sound pressure level of a working environment where the sound absorption material lies when the sound absorption material works.

S2: according to formula

${C_{a\; 2} = \frac{V_{2}}{\rho \; C_{0}^{2}}},$

calculating an equivalent acoustic capacitance C_(a2) of the second cavity 20 and a corresponding acoustic impedance

$Z_{a\; 2{(\omega)}} = \frac{1}{\omega \; C_{a\; 2}}$

at a

different frequency, wherein:

V₂ is a volume of the second cavity 20,

ρ is air density,

C₀ is sound speed.

Measuring a sound pressure P_(11(ω)) in the first cavity 10 at this time via the first sound pickup sensor 60, and measuring a sound pressure P_(21(ω)) in the second cavity 20 at this time via the second sound pickup sensor 62.

S3: putting the equivalent acoustic capacitance C_(a2) of the second cavity 20, the sound pressure P_(11(ω)) in the first cavity 10, and the sound pressure P_(21(ω)) in the second cavity 20 solved in the step S2 into formula (1) to solve the acoustic impedance Z_(ref(ω)) of the slit channel 30.

S4: placing the sound absorption material 40 to be tested in the second cavity 20, measuring a sound pressure P_(12(ω)) in the first cavity 10 at this time via the first sound pickup sensor 60, measuring a sound pressure P_(22(ω)) in the second cavity 20 at this time via the second sound pickup sensor 62, then putting Z_(ref(ω)) solved in step S3 into formula (3) to solve a uniform acoustic impedance Z_(L (ω)) after the sound absorption material 40 is placed in the second cavity 20.

S5: putting Z_(L (ω)) solved in step S4 into formula (2) to solve an equivalent acoustic capacitance C_(dut) of the sound absorption material 40,

$\begin{matrix} \begin{matrix} {Z_{L{(\omega)}} = \frac{\frac{1}{\omega \; C_{a\; 2}} \times \frac{1}{\omega \; C_{dut}}}{\frac{1}{\omega \; C_{a\; 2}} + \frac{1}{\omega \; C_{dut}}}} \\ {= \frac{1}{{\omega \; C_{dut}} + {\omega \; C_{a\; 2}}}} \end{matrix} & {{formula}\mspace{14mu} (2)} \end{matrix}$

The following is solved:

$\begin{matrix} {C_{dut} = \frac{1 - {\omega \; {C_{a\; 2} \cdot Z_{L{(\omega)}}}}}{\omega \; Z_{L{(\omega)}}}} \\ {= {\frac{1}{\omega \; Z_{L{(\omega)}}} - C_{a\; 2}}} \end{matrix}$

Putting the solved C_(dut) into formula V_(dut)=ρC₀ ²C_(dut) to solve a capacity expansion amount V_(dut) of the sound absorption material 40,

${V_{dut} = {\rho \; {C_{0}^{2}\left( {\frac{1}{\omega \; Z_{L{(\omega)}}} - C_{a\; 2}} \right)}}},$

It is feasible to, according to the solved equivalent acoustic capacitance C_(dut) and capacity expansion amount V_(dut) of the sound absorption material 40, determine the impedance characteristic and expansion performance of the sound absorption material 40, and thereby judging whether the tested sound absorption material 40 satisfies technical requirements of the acoustic product.

As known from the above, the device and method for testing impedance characteristic and expansion performance of a sound absorption material according to the present application solve the technical difficulty of failure to test the impedance characteristic and expansion performance of the sound absorption material. With the device and method of the present application, it is unnecessary to install the sound absorption material in the acoustic product to test whether the performance of the acoustic product is improved to judge whether the sound absorption material meets technical requirements of the acoustic product when the sound absorption material is selected for the acoustic product. Technicians may select a suitable sound absorption material for the acoustic product very quickly only according to the measured parameters of the sound absorption material such as equivalent acoustic capacitance and capacity expansion amount, thereby substantially shortening the development cycle of a new product, and meanwhile eliminating large waste of manpower and material resources, greatly reducing production costs of the acoustic product and bringing about larger economic benefits to the enterprises.

Technical terms (e.g., the first cavity and the second cavity) denoted by a serial number involved in the description are only intended to distinguish technical features, and does not represent positional relationship, assembling order, and operation order of the technical features.

The present application is not limited to the above specific embodiments. Diverse variations made by those having ordinary skill in the art starting from the above concept without making any inventive efforts all fall within the protection scope of the present application.

While at least one exemplary embodiment has been presented in the foregoing detailed description, it should be appreciated that a vast number of variations exist. It should also be appreciated that the exemplary embodiment or exemplary embodiments are only examples, and are not intended to limit the scope, applicability, or configuration of the invention in any way. Rather, the foregoing detailed description will provide those skilled in the art with a convenient road map for implementing an exemplary embodiment, it being understood that various changes may be made in the function and arrangement of elements described in an exemplary embodiment without departing from the scope of the invention as set forth in the appended claims and their legal equivalents. 

1. A device for testing impedance characteristic and expansion performance of a sound absorption material, comprises: a first cavity and a second cavity which are both sealed, the first cavity being communicated with the second cavity through a slit channel, wherein the second cavity is used for placing a sound absorption material therein; a sound excitation source whose sounding face is located in the first cavity and used to provide a testing sound pressure; two sound pickup sensors whose sound pickup surfaces are respectively arranged in the first cavity and the second cavity and which are respectively used to detect sound pressure in the first cavity and the second cavity; a material for enclosing the first cavity and the second cavity is a hard sound insulation material.
 2. The device for testing impedance characteristic and expansion performance of the sound absorption material according to claim 1, wherein the first cavity and the second cavity each are a cavity with a regular shape.
 3. The device for testing impedance characteristic and expansion performance of the sound absorption material according to claim 2, wherein the sounding face of the sound excitation source flushes with a surface of an inner wall of the first cavity.
 4. The device for testing impedance characteristic and expansion performance of the sound absorption material according to claim 3, wherein the sound excitation source is a speaker.
 5. The device for testing impedance characteristic and expansion performance of the sound absorption material according to claim 3, wherein the sound pickup sensor is a microphone.
 6. The device for testing impedance characteristic and expansion performance of the sound absorption material according to claim 3, wherein the sound isolation material is one of metal, bakelite and acrylic.
 7. A method for testing impedance characteristic and expansion performance of a sound absorption material by using the device according to claim 1, wherein the method comprises the following steps: S1: adjusting a voltage of the sound excitation source to enable the sound pressure in the second cavity to satisfy a sound pressure level needed by the test; S2: Measuring a sound pressure P_(11(ω)) in the first cavity via the first sound pickup sensor, and measuring a sound pressure P_(21(ω)) in the second cavity via the second sound pickup sensor; solving an equivalent acoustic capacitance C_(a2) and an acoustic impedance Z_(a2(ω)) of the second cavity according to formula ${C_{a\; 2} = {{\frac{V_{2}}{\rho \; C_{0}^{2}}\mspace{14mu} {and}\mspace{14mu} Z_{a\; 2{(\omega)}}} = \frac{1}{\omega \; C_{a\; 2}}}},$ wherein V₂ is a volume of the second cavity, ρ is air density, C⁰ is a sound speed, and ω is an angular speed; S3: obtaining formula $Z_{{ref}{(\omega)}} = \frac{P_{11{(\omega)}} - P_{21{(\omega)}}}{P_{21{(\omega)}} \times \omega \; C_{a\; 2}}$ according to an acoustic circuit that is equivalent to the device when the sound absorption material is not placed in the device, and putting the equivalent acoustic capacitance C_(a2) solved from step S2 into the formula to solve an acoustic impedance Z_(ref (ω)) of the slit channel; S4: placing the sound absorption material to be tested in the second cavity, measuring a sound pressure P_(12(ω)) in the first cavity via the first sound pickup sensor, and measuring a sound pressure P_(22(ω)) in the second cavity via the second sound pickup sensor, obtaining formula $Z_{L{(\omega)}} = \frac{P_{22{(\omega)}}}{\frac{P_{12{(\omega)}} - P_{22{(\omega)}}}{Z_{{ref}{(\omega)}}}}$ according to the acoustic circuit that is equivalent to the device after the sound absorption material is placed in the device, putting the acoustic impedance Z_(ref(ω)) of the slit channel solved in step S3 into the formula to solve a uniform acoustic impedance Z_(L (ω)) after the sound absorption material is placed in the second cavity; S5: obtaining formula $Z_{L{(\omega)}} = \frac{\frac{1}{\omega \; C_{a\; 2}} \times \frac{1}{\omega \; C_{dut}}}{\frac{1}{\omega \; C_{a\; 2}} + \frac{1}{\omega \; C_{dut}}}$ according to the acoustic circuit that is equivalent to the device after the sound absorption material is placed in the device, and solving an equivalent acoustic capacitance C_(dut) of the sound absorption material; and then solving a capacity expansion amount V_(dut) of the sound absorption material according to the formula V_(dut) =ρC₀ ²C_(dut), and thereby judging the impedance characteristic and expansion performance of the sound absorption material.
 8. The method for testing impedance characteristic and expansion performance of a sound absorption material according to claim 7, wherein a sound pressure level needed by the test in step S1 is a sound pressure level of an actual working environment of the sound absorption material. 